{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:S4JZLIC5QYSWIRVM7RDSYXDCQ2","short_pith_number":"pith:S4JZLIC5","schema_version":"1.0","canonical_sha256":"971395a05d86256446acfc472c5c62869029b10652edcc95b96ea5d2bafe457f","source":{"kind":"arxiv","id":"hep-th/0512325","version":1},"attestation_state":"computed","paper":{"title":"Thermodynamics of Noncritical M-Theory and the Topological A-Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Cynthia A. Keeler, Petr Horava","submitted_at":"2005-12-28T04:38:13Z","abstract_excerpt":"In hep-th/0508024, noncritical M-theory for two-dimensional Type 0A and 0B strings was defined in terms of a double-scaled theory of nonrelativistic fermions in 2+1 dimensions. Here we study this noncritical M-theory at finite temperature. We derive the exact expression for the free energy of its vacuum solution, as a function of a coupling constant $g_M$ and the radius $R$ of the thermal circle. We show that at high temperature, the theory is effectively described by another M-theory solution, whose effective loop-counting coupling scales in a novel way characteristic of M-theory, as $T^3$. O"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"hep-th/0512325","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2005-12-28T04:38:13Z","cross_cats_sorted":[],"title_canon_sha256":"f070320656071bdbca976ee9e18c833f79d2abf9435c1c3a93079c1bfafa97ee","abstract_canon_sha256":"2e732021003539addaf0d3e76ff10c672928c4da56821c2f00779016a51978d3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:19:55.007361Z","signature_b64":"OxmK7cUsJRX8QStRj1vvbg7eKkW8RKPwYM/xBmoknISt2gC6co+QS+G2TFfJdTMg0XUSvZpeVW6VT2bMbCQ4DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"971395a05d86256446acfc472c5c62869029b10652edcc95b96ea5d2bafe457f","last_reissued_at":"2026-07-04T15:19:55.006708Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:19:55.006708Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermodynamics of Noncritical M-Theory and the Topological A-Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Cynthia A. Keeler, Petr Horava","submitted_at":"2005-12-28T04:38:13Z","abstract_excerpt":"In hep-th/0508024, noncritical M-theory for two-dimensional Type 0A and 0B strings was defined in terms of a double-scaled theory of nonrelativistic fermions in 2+1 dimensions. Here we study this noncritical M-theory at finite temperature. We derive the exact expression for the free energy of its vacuum solution, as a function of a coupling constant $g_M$ and the radius $R$ of the thermal circle. We show that at high temperature, the theory is effectively described by another M-theory solution, whose effective loop-counting coupling scales in a novel way characteristic of M-theory, as $T^3$. O"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0512325","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-th/0512325/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0512325","created_at":"2026-07-04T15:19:55.006775+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0512325v1","created_at":"2026-07-04T15:19:55.006775+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0512325","created_at":"2026-07-04T15:19:55.006775+00:00"},{"alias_kind":"pith_short_12","alias_value":"S4JZLIC5QYSW","created_at":"2026-07-04T15:19:55.006775+00:00"},{"alias_kind":"pith_short_16","alias_value":"S4JZLIC5QYSWIRVM","created_at":"2026-07-04T15:19:55.006775+00:00"},{"alias_kind":"pith_short_8","alias_value":"S4JZLIC5","created_at":"2026-07-04T15:19:55.006775+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/S4JZLIC5QYSWIRVM7RDSYXDCQ2","json":"https://pith.science/pith/S4JZLIC5QYSWIRVM7RDSYXDCQ2.json","graph_json":"https://pith.science/api/pith-number/S4JZLIC5QYSWIRVM7RDSYXDCQ2/graph.json","events_json":"https://pith.science/api/pith-number/S4JZLIC5QYSWIRVM7RDSYXDCQ2/events.json","paper":"https://pith.science/paper/S4JZLIC5"},"agent_actions":{"view_html":"https://pith.science/pith/S4JZLIC5QYSWIRVM7RDSYXDCQ2","download_json":"https://pith.science/pith/S4JZLIC5QYSWIRVM7RDSYXDCQ2.json","view_paper":"https://pith.science/paper/S4JZLIC5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0512325&json=true","fetch_graph":"https://pith.science/api/pith-number/S4JZLIC5QYSWIRVM7RDSYXDCQ2/graph.json","fetch_events":"https://pith.science/api/pith-number/S4JZLIC5QYSWIRVM7RDSYXDCQ2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/S4JZLIC5QYSWIRVM7RDSYXDCQ2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/S4JZLIC5QYSWIRVM7RDSYXDCQ2/action/storage_attestation","attest_author":"https://pith.science/pith/S4JZLIC5QYSWIRVM7RDSYXDCQ2/action/author_attestation","sign_citation":"https://pith.science/pith/S4JZLIC5QYSWIRVM7RDSYXDCQ2/action/citation_signature","submit_replication":"https://pith.science/pith/S4JZLIC5QYSWIRVM7RDSYXDCQ2/action/replication_record"}},"created_at":"2026-07-04T15:19:55.006775+00:00","updated_at":"2026-07-04T15:19:55.006775+00:00"}